Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. |
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Page 6
Volume 8 L D Landau, E.M. Lifshitz, L. P. Pitaevskii. charge distribution on the conductors undergoes an infinitesimal change ( the total charge on each conductor remaining unaltered ) , in which the charges may penetrate into the ...
Volume 8 L D Landau, E.M. Lifshitz, L. P. Pitaevskii. charge distribution on the conductors undergoes an infinitesimal change ( the total charge on each conductor remaining unaltered ) , in which the charges may penetrate into the ...
Page 7
... charge e ( regarding the latter as a very small conductor ) . In one state the charge e is present , the charges on the conductors are e , and their potentials are zero . In the other state the charge e is zero , and one of the ...
... charge e ( regarding the latter as a very small conductor ) . In one state the charge e is present , the charges on the conductors are e , and their potentials are zero . In the other state the charge e is zero , and one of the ...
Page 9
... charge e is given by - σ = 1 Гаф 4π . δη e a = 2π μ3 ( 3.2 ) It is easy to see that the total charge on the plane is fodf = −e , as it should be . The total charge induced on an originally uncharged insulated conductor by other charges ...
... charge e is given by - σ = 1 Гаф 4π . δη e a = 2π μ3 ( 3.2 ) It is easy to see that the total charge on the plane is fodf = −e , as it should be . The total charge induced on an originally uncharged insulated conductor by other charges ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid equation expression external field ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ